Probing non-holomorphic MSSM via precision constraints, dark matter and LHC data

被引:0
作者
Utpal Chattopadhyay
Abhishek Dey
机构
[1] Indian Association for the Cultivation of Science,Department of Theoretical Physics
[2] Maulana Azad College,undefined
[3] Government of West Bengal,undefined
来源
Journal of High Energy Physics | / 2016卷
关键词
Supersymmetry Phenomenology;
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摘要
In this analysis we explore the phenomenological constraints of models with non-holomorphic soft SUSY breaking terms in a beyond the MSSM scenario having identical particle content. The model referred as NHSSM shows various promising features like the possibility of a strong reduction in electroweak fine-tuning even for a scenario of a heavy higgsino type of LSP, a fact that is unavailable in pMSSM models. The other important aspect is satisfying the muon g − 2 data even for a small tan β via a small value of coupling Aμ′ associated with the tri-linear non-holomorphic soft term. Thus, a large SUSY contribution to muon g − 2 is possible even for a significantly large smuon mass mμ˜1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {m_{\tilde{\mu}}}_1 $$\end{document}. The Higgs mass radiative corrections are contributed by both the holomorphic and non-holomorphic trilinear soft parameters At and At′, thus diluting the requirement to have a larger At to satisfy the Higgs mass data. The model also provides with valid parameter space satisfying the constraint of Br(B → Xs + γ) for large values of tan β, a scenario unfavourable in pMSSM.
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[41]  
Chakraborti M(2013)Naturalness of Light Neutralino Dark Matter in pMSSM after LHC, XENON100 and Planck Data Phys. Rev. D 87 035022-undefined
[42]  
Chattopadhyay U(2012)Interpreting the LHC Higgs Search Results in the MSSM Phys. Lett. B 716 214-undefined
[43]  
Choudhury A(2010)The Higgs sector of the phenomenological MSSM in the light of the Higgs boson discovery Comput. Phys. Commun. 181 1077-undefined
[44]  
Datta A(2011)Implication of a Higgs boson at 125 GeV within the stochastic superspace framework Comput. Phys. Commun. 182 808-undefined
[45]  
Poddar S(2012)The top quark and Higgs boson masses and the stability of the electroweak vacuum Comput. Phys. Commun. 183 2458-undefined
[46]  
Chakraborti M(2014)From Superpotential to Model Files for FeynArts and CalcHep/CompHEP Eur. Phys. J. C 74 2992-undefined
[47]  
Chattopadhyay U(2013)Automatic Calculation of supersymmetric Renormalization Group Equations and Self Energies Comput. Phys. Commun. 184 1792-undefined
[48]  
Choudhury A(2014)SPheno 3.1: Extensions including flavour, CP-phases and models beyond the MSSM Comput. Phys. Commun. 185 1773-undefined
[49]  
Datta A(2013)A Flavor Kit for BSM models JHEP 01 061-undefined
[50]  
Poddar S(2014)SARAH 3.2: Dirac Gauginos, UFO output and more JHEP 11 161-undefined